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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 9 (1997), S. 3817-3825 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Scaling exponents of the longitudinal and transversal velocity structure functions in numerical Navier–Stokes turbulence simulations with Taylor–Reynolds numbers up to Reλ=110 are determined by the extended self similarity method. We find significant differences in the degree of intermittency: For the sixth moments the scaling corrections to the classical Kolmogorov expectations are δξ6L=−0.21±0.01 and δξ6T=−0.43±0.01, respectively, independent of Reλ. Also the generalized extended self similarity exponents ρp,q=δξp/δξq differ significantly for the longitudinal and transversal structure functions. Within the She–Leveque model this means that longitudinal and transversal fluctuations obey different types of hierarchies of the moments. Moreover, the She–Leveque model hierarchy parameters βL and βT show small but significant dependences on the order of the moment. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 1 (1989), S. 1021-1026 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The structure function Dθ(r) of a passive scalar, e.g., the temperature, in fully developed turbulence is calculated directly from the Navier–Stokes and diffusion equations. A variable range decomposition of the turbulent flow field is used to derive a parameter-free equation for Dθ(r), valid for all values of r and all (molecular) Prandtl numbers Pr, thus representing a unified description of passive scalar diffusion. Here Dθ(r) shows three distinct ranges of r behavior; we give the Pr dependence of the borders between them. In the inertial range the turbulent Prandtl number is Prturb =0.40.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 8 (1996), S. 1814-1819 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We analyze the mechanism that determines the boundary of stability in Taylor–Couette flow. By simple physical argument we derive an analytic expression to approximate the stability line for all radius ratios and all speed ratios, for co- and counterrotating cylinders. The expression includes viscosity and so generalizes Rayleigh's criterion. We achieve agreement with linear stability theory and with experiments in the whole parameter space. Explicit formulae are given for limiting cases. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 6 (1994), S. 3823-3832 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The stability of time modulated Taylor–Couette flow with co- and counter-rotating cylinders and modulated inner cylinder velocity is investigated. The mean velocities of the inner and outer cylinders are chosen to be in constant relative distance to the stability border of nonmodulated Taylor–Couette flow and the inner cylinder velocity is periodically modulated. The critical modulation amplitude, which leads to linear instability of the modulated laminar flow, is calculated with numerically integrated Floquet theory, as well as with perturbation theory. The critical modulation amplitude as a function of the outer cylinder Reynolds number has a rich structure for counter-rotating cylinders, which is open to experimental test. The critical modulation amplitude decreases monotonically with increasing rotation frequency for corotating cylinders. © 1994 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 6 (1994), S. 611-617 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The deviations δζm ("intermittency corrections'') from classical ("K41'') scaling ζm=m/3 of the mth moments 〈||u(p)||m〉 in high Reynolds number turbulence are calculated, extending a method to approximately solve the Navier–Stokes equation described earlier. It is suggested to introduce the notion of scale resolved intermittency corrections δζm(p), because these δζm(p) are found to be large in the viscous subrange, moderate in the nonuniversal stirring subrange but, surprisingly, extremely small if not zero in the inertial subrange. If ISR intermittency corrections persisted in experiment up to the large Reynolds number limit, it would show by calculation that this could be due to the opening of phase space for larger wave vectors. In the higher order velocity moments 〈||u(p)||m〉 the crossover between inertial and viscous subrange is (10ηm/2)−1, thus the inertial subrange is smaller for higher order moments.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 6 (1994), S. 3798-3798 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 3 (1991), S. 1958-1968 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A Fourier–Weierstrass decomposition of the velocity field is introduced. The admitted number of real amplitudes is 572 or 836. They are determined numerically from the Navier–Stokes equation including viscosity, driven by constant energy input stirring the largest eddies only. In another calculation, the energy input is provided by an external shear. The Reynolds number Re is about 106, the inertial range comprises about 2 decades, and there are 11 levels of successively decaying eddies. The hierarchical mode ansatz thus allows for a state of high turbulence, which usually is inaccessible numerically. Deterministic chaos is found on all scales. The mean values of the amplitudes scale with the eddy size r as rζ with ζ very near 1/3. Expected deviations δζ=ζ−1/3, as one typical signature of intermittency, are very small only, well compatible with none at all. So, despite stochasticity (chaos) in the Fourier–Weierstrass decomposition with a tractably restricted set of plane waves, intermittency in the velocity scaling cannot be found. This changes if, in addition to temporal chaos, a spatial branching of the eddy decay process is also admitted.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    [s.l.] : Macmillan Magazines Ltd.
    Nature 398 (1999), S. 402-405 
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] Ultrasonically driven gas bubbles in liquids can emit intense bursts of light when they collapse. The physical mechanism for single-bubble sonoluminescence has been much debated,. The conditions required for, and generated by, bubble collapse can be deduced within the framework of a ...
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 90 (1993), S. 1-1 
    ISSN: 1434-6036
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 182 (1964), S. 24-33 
    ISSN: 1434-601X
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract It is shown that the Boltzmann equation of a dilute gas at temperatures above condensation includingLandau's quantum corrections of the streaming term results in a real equation of state. The quantum virial coefficients are given explicitly up to the fourth. A simple prescription for the higher ones is formulated. In the binary collision approximation, which basically underlies the transport equation itself, all virial coefficients can be expressed by correlated products of the real part of the two particle forward scattering amplitude. Averaging these with the free Maxwell distribution at temperatureT one getsB(T),C(T) etc.
    Type of Medium: Electronic Resource
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